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NSR database version of April 27, 2024.

Search: Author = F.Dickmann

Found 15 matches.

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1987KR07      Phys.Rev. C36, 327 (1987)

A.T.Kruppa, R.Beck, F.Dickmann

Electromagnetic Properties of 6Li in a Cluster Model with Breathing Clusters

NUCLEAR STRUCTURE 2H; calculated structure function, rms radius, binding energy. 4He; calculated binding energy, rms radius, charge form factor. 6Li; calculated binding energy, rms radius, B(E2), level < E >. Generator coordinate method.

NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated charge, magnetic form factors. Microscopic α+d cluster model.

doi: 10.1103/PhysRevC.36.327
Citations: PlumX Metrics

1987LO16      Nucl.Phys. A474, 451 (1987)

R.G.Lovas, A.T.Kruppa, R.Beck, F.Dickmann

Fragmentation Properties of 6Li

NUCLEAR REACTIONS 6Li(p, pd), E=670, 590 MeV; 6Li(α, 2α), E=700 MeV; 6Li(p, p3He), E not given; calculated fragmentation strengths.

NUCLEAR STRUCTURE 6Li; calculated α+d, t+3He cluster fragmentation amplitudes. 3,2H, 3,4He; calculated rms charge radii, binding energies.

doi: 10.1016/0375-9474(87)90626-9
Citations: PlumX Metrics

1986KR12      Phys.Lett. 179B, 317 (1986)

A.T.Kruppa, R.G.Lovas, R.Beck, F.Dickmann

Breathing Cluster Model for Nuclei of Two s-Wave Clusters

NUCLEAR STRUCTURE 5He, 6,7Li, 7,8Be; calculated binding energies. 6Li; calculated charge form factor square, α-d fragmentation strength. Breathing model, two s-wave clusters.

doi: 10.1016/0370-2693(86)90484-3
Citations: PlumX Metrics

1986NA09      Phys.Rev. C34, 218 (1986)

A.A.Naqvi, F.Kappeler, F.Dickmann, R.Muller

Fission Fragment Properties in Fast-Neutron-Induced Fission of 237Np

NUCLEAR REACTIONS 237Np(n, F), E=0.8, 5.55 MeV; measured correlated fission fragment kinetic energies, velocities; deduced fragment mass and energy distributions, variances, average neutron multiplicities.

doi: 10.1103/PhysRevC.34.218
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21834.

1985BE60      Nucl.Phys. A446, 703 (1985)

R.Beck, F.Dickmann, R.G.Lovas

Quasielastic Cluster Knock-Out Reactions and the Microscopic Cluster Model

NUCLEAR REACTIONS 6Li(p, pd), (α, 2α), E not given; calculated spectroscopic amplitude vs α-d relative momentum; deduced Sα. Quasielastic cluster knockout reactions.

NUCLEAR STRUCTURE 6Li; calculated fragmentation amplitude, Sα. Microscopic cluster model, (α+d), (5He+p) clusters.

doi: 10.1016/0375-9474(85)90638-4
Citations: PlumX Metrics

1984BE37      Phys.Rev. C30, 1044 (1984)

R.Beck, F.Dickmann, A.T.Kruppa

Cluster Model with Breathing Clusters: Dynamical distortion effects in 6Li

NUCLEAR STRUCTURE 6Li; calculated ground state energy, deuteron cluster size. Generator coordinate method.

doi: 10.1103/PhysRevC.30.1044
Citations: PlumX Metrics

1984MU05      Phys.Rev. C 29, 885 (1984)

R.Muller, A.A.Naqvi, F.Kappeler, F.Dickmann

Fragment velocities, energies, and masses from fast neutron induced fission of 235U

NUCLEAR REACTIONS 235U(n, F), E=0.5, 5.55 MeV; measured fission products, En, In; deduced fragment velocities and masses, total kinetic energies and their variances, the number of prompt fission neutrons.

doi: 10.1103/physrevc.29.885
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21834.

1976CH26      Phys.Rev.Lett. 37, 1738 (1976)

E.F.Chaffin, F.Dickmann

Validity of the Adiabatic Cranking Model When Applied to Fission

NUCLEAR STRUCTURE 236U; calculated fission saddle points.

doi: 10.1103/PhysRevLett.37.1738
Citations: PlumX Metrics

1975CH24      Nucl.Phys. A251, 65 (1975)

E.F.Chaffin, F.Dickmann, N.V.V.J.Swamy

A Two-Center Relativistic Oscillator Model and its Application in Estimation of Shell Corrections

NUCLEAR STRUCTURE 208Pb; calculated levels.

doi: 10.1016/0375-9474(75)90701-0
Citations: PlumX Metrics

1974DI19      Z.Phys. 271, 417 (1974)

F.Dickmann, K.Dietrich

Coexistence and Mixing of Spherical and Deformed States in the Region of Light Hg-Isotopes

NUCLEAR STRUCTURE 184,186Hg; calculated levels, β; deduced existence of shape isomers.

doi: 10.1007/BF02126197
Citations: PlumX Metrics

1973DI12      Z.Phys. 263, 211 (1973)

F.Dickmann, K.Dietrich

Variable Collective Inertia and the Transition from Spherical to Deformed Shapes in the Hg-Isotopes

NUCLEAR STRUCTURE 182,185,186,187,188,192,194Hg; calculated deformation energies.

doi: 10.1007/BF01392563
Citations: PlumX Metrics

1972DI03      Phys.Lett. 38B, 207 (1972)

F.Dickmann, V.Metag, R.Repnow

Predicted Region of Oblate Deformation Around 72Kr

NUCLEAR STRUCTURE 71,72Kr; calculated potential energy surfaces, deformation energy. Structinsky formalism.

doi: 10.1016/0370-2693(72)90380-2
Citations: PlumX Metrics

1971DI10      Phys.Lett. 35B, 467 (1971)

F.Dickmann

Single-Particle Model for Strongly Deformed Nuclei

NUCLEAR REACTIONS 58Ni(n, γ), E=thermal; calculated Iγ. 59Ni resonance deduced level-width.

doi: 10.1016/0370-2693(71)90370-4
Citations: PlumX Metrics

1971ME02      Phys.Lett. 34B, 257 (1971)

V.Metag, R.Repnow, P.Von Brentano, F.Dickmann, K.Dietrich

A Secondary Minimum in the Potential Energy Surface of 40Ca

NUCLEAR STRUCTURE 40Ca; calculated potential energy surface; deduced secondary minima.

doi: 10.1016/0370-2693(71)90597-1
Citations: PlumX Metrics

1970AN28      Nucl.Phys. A159, 337 (1970)

B.L.Andersen, F.Dickmann, K.Dietrich

Potential Landscape for Fissioning Nuclei (I). General Method, Symmetric Shapes

NUCLEAR STRUCTURE 226Ra, 236U; calculated deformation energy, potential energy vs deformation. Strutinski method.

doi: 10.1016/0375-9474(70)90712-8
Citations: PlumX Metrics

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